# Electronic Supplementary Material (ESI) for ChemComm.
# This journal is © The Royal Society of Chemistry 2019

####################################################################### 
# 
# This file contains crystal structure data downloaded from the 
# Cambridge Structural Database (CSD) hosted by the Cambridge 
# Crystallographic Data Centre (CCDC).
# 
# Full information about CCDC data access policies and citation 
# guidelines are available at http://www.ccdc.cam.ac.uk/access/V1 
# 
# Audit and citation data items may have been added by the CCDC. 
# Please retain this information to preserve the provenance of 
# this file and to allow appropriate attribution of the data. 
# 
#######################################################################

data_sm_ird0257_0m
_audit_block_doi                 10.5517/ccdc.csd.cc21f16r
_database_code_depnum_ccdc_archive 'CCDC 1889363'
loop_
_audit_author_name
_audit_author_address
'Rajender Reddy Leleti'
;Piramal 
India
;
_audit_update_record             
;
2019-01-08 deposited with the CCDC.	2019-03-07 downloaded from the CCDC.
;
_audit_creation_date             2018-10-10
_audit_creation_method           
;
Olex2 1.2
(compiled 2018.05.29 svn.r3508 for OlexSys, GUI svn.r5506)
;
_shelx_SHELXL_version_number     2018/1
_chemical_name_common            ?
_chemical_name_systematic        ?
_chemical_formula_moiety         'C14 H21 N O S2'
_chemical_formula_sum            'C14 H21 N O S2'
_chemical_formula_weight         283.44
_chemical_absolute_configuration rm
_chemical_melting_point          ?
loop_
_atom_type_symbol
_atom_type_description
_atom_type_scat_dispersion_real
_atom_type_scat_dispersion_imag
_atom_type_scat_source
C C 0.0033 0.0016 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
H H 0.0000 0.0000 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
N N 0.0061 0.0033 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
O O 0.0106 0.0060 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'
S S 0.1246 0.1234 'International Tables Vol C Tables 4.2.6.8 and 6.1.1.4'

_shelx_space_group_comment       
;
The symmetry employed for this shelxl refinement is uniquely defined
by the following loop, which should always be used as a source of
symmetry information in preference to the above space-group names.
They are only intended as comments.
;
_space_group_crystal_system      orthorhombic
_space_group_IT_number           19
_space_group_name_H-M_alt        'P 21 21 21'
_space_group_name_Hall           'P 2ac 2ab'
loop_
_space_group_symop_operation_xyz
'x, y, z'
'-x+1/2, -y, z+1/2'
'-x, y+1/2, -z+1/2'
'x+1/2, -y+1/2, -z'

_cell_length_a                   8.5013(8)
_cell_length_b                   12.0985(12)
_cell_length_c                   15.0956(17)
_cell_angle_alpha                90
_cell_angle_beta                 90
_cell_angle_gamma                90
_cell_volume                     1552.6(3)
_cell_formula_units_Z            4
_cell_measurement_reflns_used    6816
_cell_measurement_temperature    296(2)
_cell_measurement_theta_max      25.05
_cell_measurement_theta_min      2.70
_shelx_estimated_absorpt_T_max   ?
_shelx_estimated_absorpt_T_min   ?
_exptl_absorpt_coefficient_mu    0.332
_exptl_absorpt_correction_T_max  0.7452
_exptl_absorpt_correction_T_min  0.6820
_exptl_absorpt_correction_type   multi-scan
_exptl_absorpt_process_details   'SADABS-2014/4 (Bruker,2014/4)'
_exptl_absorpt_special_details   ?
_exptl_crystal_colour            colorless
_exptl_crystal_density_diffrn    1.213
_exptl_crystal_density_meas      ?
_exptl_crystal_density_method    ?
_exptl_crystal_description       block
_exptl_crystal_F_000             608
_exptl_crystal_size_max          0.25
_exptl_crystal_size_mid          0.22
_exptl_crystal_size_min          0.22
_exptl_transmission_factor_max   ?
_exptl_transmission_factor_min   ?
_diffrn_reflns_av_R_equivalents  0.0340
_diffrn_reflns_av_unetI/netI     0.0236
_diffrn_reflns_Laue_measured_fraction_full 0.999
_diffrn_reflns_Laue_measured_fraction_max 0.998
_diffrn_reflns_limit_h_max       10
_diffrn_reflns_limit_h_min       -10
_diffrn_reflns_limit_k_max       14
_diffrn_reflns_limit_k_min       -14
_diffrn_reflns_limit_l_max       18
_diffrn_reflns_limit_l_min       -16
_diffrn_reflns_number            12105
_diffrn_reflns_point_group_measured_fraction_full 0.999
_diffrn_reflns_point_group_measured_fraction_max 0.998
_diffrn_reflns_theta_full        25.114
_diffrn_reflns_theta_max         25.114
_diffrn_reflns_theta_min         2.157
_diffrn_ambient_temperature      296.15
_diffrn_detector_area_resol_mean ?
_diffrn_measured_fraction_theta_full 0.999
_diffrn_measured_fraction_theta_max 0.998
_diffrn_measurement_device_type  'Bruker APEX-II CCD'
_diffrn_measurement_method       'φ and ω scans'
_diffrn_radiation_type           MoK\a
_diffrn_radiation_wavelength     0.71073
_diffrn_source                   ?
_diffrn_standards_number         0
_reflns_Friedel_coverage         0.724
_reflns_Friedel_fraction_full    0.998
_reflns_Friedel_fraction_max     0.998
_reflns_number_gt                2626
_reflns_number_total             2765
_reflns_special_details          
;
 Reflections were merged by SHELXL according to the crystal
 class for the calculation of statistics and refinement.
 
 _reflns_Friedel_fraction is defined as the number of unique
 Friedel pairs measured divided by the number that would be
 possible theoretically, ignoring centric projections and
 systematic absences.
;
_reflns_threshold_expression     'I > 2σ(I)'
_computing_cell_refinement       'SAINT v8.34A (Bruker, 2013)'
_computing_data_collection       'Bruker APEX-II'
_computing_data_reduction        'SAINT v8.34A (Bruker, 2013)'
_computing_molecular_graphics    'Olex2 (Dolomanov et al., 2009)'
_computing_publication_material  'Olex2 (Dolomanov et al., 2009)'
_computing_structure_refinement  'ShelXL (Sheldrick, 2015)'
_computing_structure_solution    'XT (Sheldrick, 2015)'
_refine_diff_density_max         0.201
_refine_diff_density_min         -0.310
_refine_diff_density_rms         0.062
_refine_ls_abs_structure_details 
;
 Flack x determined using 1071 quotients [(I+)-(I-)]/[(I+)+(I-)]
 (Parsons, Flack and Wagner, Acta Cryst. B69 (2013) 249-259).
;
_refine_ls_abs_structure_Flack   0.04(3)
_refine_ls_extinction_coef       .
_refine_ls_extinction_method     none
_refine_ls_goodness_of_fit_ref   1.074
_refine_ls_hydrogen_treatment    constr
_refine_ls_matrix_type           full
_refine_ls_number_parameters     202
_refine_ls_number_reflns         2765
_refine_ls_number_restraints     61
_refine_ls_R_factor_all          0.0362
_refine_ls_R_factor_gt           0.0341
_refine_ls_restrained_S_all      1.067
_refine_ls_shift/su_max          0.000
_refine_ls_shift/su_mean         0.000
_refine_ls_structure_factor_coef Fsqd
_refine_ls_weighting_details     
'w=1/[σ²(Fo²)+(0.0652P)²+0.0844P] where P=(Fo²+2Fc²)/3'
_refine_ls_weighting_scheme      calc
_refine_ls_wR_factor_gt          0.0918
_refine_ls_wR_factor_ref         0.0944
_refine_special_details          ?
_olex2_refinement_description    
;
1. Fixed Uiso
 At 1.2 times of:
  All C(H) groups, All C(H,H) groups
 At 1.5 times of:
  All C(H,H,H) groups
2. Restrained distances
 S2A-C12 \\sim S2B-C12
 with sigma of 0.02
 S2A-C14A \\sim S2B-C14B
 with sigma of 0.02
 C11A-C12 \\sim C11B-C12
 with sigma of 0.02
 C11A-C13A \\sim C11B-C13B
 with sigma of 0.02
 C13A-C14A \\sim C13B-C14B
 with sigma of 0.02
 S2A-C13A \\sim S2B-C13B
 with sigma of 0.04
 C11A-C14A \\sim C11B-C14B
 with sigma of 0.04
 C12-C13A \\sim C12-C13B
 with sigma of 0.04
 C12-C14A \\sim C12-C14B
 with sigma of 0.04
3. Rigid body (RIGU) restrains
 S2A, S2B, C11A, C11B, C12, C13A, C13B, C14A, C14B
 with sigma for 1-2 distances of 0.02 and sigma for 1-3 distances of 0.02
4. Others
 Fixed Sof: S2A(0.58654) S2B(0.41346) C11A(0.58654) H11A(0.58654)
 C13A(0.58654) H13A(0.58654) C14A(0.58654) H14A(0.58654) C11B(0.41346)
 H11B(0.41346) C13B(0.41346) H13B(0.41346) C14B(0.41346) H14B(0.41346)
5.a Ternary CH refined with riding coordinates:
 C1(H1)
5.b Secondary CH2 refined with riding coordinates:
 C4(H4A,H4B), C5(H5A,H5B), C8(H8A,H8B), C10(H10A,H10B)
5.c Aromatic/amide H refined with riding coordinates:
 C11A(H11A), C13A(H13A), C14A(H14A), C11B(H11B), C13B(H13B), C14B(H14B)
5.d Idealised Me refined as rotating group:
 C6(H6A,H6B,H6C), C7(H7A,H7B,H7C), C9(H9A,H9B,H9C)
;
_atom_sites_solution_hydrogens   geom
_atom_sites_solution_primary     dual
_atom_sites_solution_secondary   ?
loop_
_atom_site_label
_atom_site_type_symbol
_atom_site_fract_x
_atom_site_fract_y
_atom_site_fract_z
_atom_site_U_iso_or_equiv
_atom_site_adp_type
_atom_site_occupancy
_atom_site_site_symmetry_order
_atom_site_calc_flag
_atom_site_refinement_flags_posn
_atom_site_refinement_flags_adp
_atom_site_refinement_flags_occupancy
_atom_site_disorder_assembly
_atom_site_disorder_group
S1 S 0.52658(8) 0.61449(5) 0.54320(4) 0.0488(2) Uani 1 1 d . . . . .
S2A S 0.7531(6) 0.3152(5) 0.6616(3) 0.0759(15) Uani 0.5865 1 d D U P A 1
S2B S 0.5675(12) 0.2000(7) 0.5665(6) 0.074(2) Uani 0.4135 1 d D U P A 2
O1 O 0.3902(2) 0.58857(16) 0.48563(13) 0.0603(5) Uani 1 1 d . . . . .
N1 N 0.5437(3) 0.51742(16) 0.62245(13) 0.0487(5) Uani 1 1 d . . . . .
C1 C 0.4736(3) 0.40440(18) 0.60841(15) 0.0463(5) Uani 1 1 d . . . . .
H1 H 0.409163 0.402142 0.554623 0.056 Uiso 1 1 calc R . . . .
C2 C 0.7020(3) 0.5897(2) 0.47482(18) 0.0550(6) Uani 1 1 d . . . . .
C3 C 0.3701(3) 0.4222(2) 0.69255(18) 0.0547(7) Uani 1 1 d . . . . .
C4 C 0.3730(4) 0.3406(3) 0.7699(2) 0.0730(9) Uani 1 1 d . . . . .
H4A H 0.447021 0.280337 0.762171 0.088 Uiso 1 1 calc R . . . .
H4B H 0.386415 0.375435 0.827305 0.088 Uiso 1 1 calc R . . . .
C5 C 0.4373(4) 0.5391(3) 0.6999(2) 0.0696(8) Uani 1 1 d . . . . .
H5A H 0.360247 0.596693 0.688953 0.084 Uiso 1 1 calc R . . . .
H5B H 0.493197 0.552577 0.754838 0.084 Uiso 1 1 calc R . . . .
C6 C 0.6981(4) 0.6872(3) 0.4105(2) 0.0738(9) Uani 1 1 d . . . . .
H6A H 0.600468 0.686794 0.378604 0.111 Uiso 1 1 calc GR . . . .
H6B H 0.783991 0.681127 0.369544 0.111 Uiso 1 1 calc GR . . . .
H6C H 0.707424 0.755064 0.443124 0.111 Uiso 1 1 calc GR . . . .
C7 C 0.6881(4) 0.4809(3) 0.4261(2) 0.0753(9) Uani 1 1 d . . . . .
H7A H 0.698008 0.421048 0.467400 0.113 Uiso 1 1 calc GR . . . .
H7B H 0.770010 0.475812 0.382464 0.113 Uiso 1 1 calc GR . . . .
H7C H 0.587517 0.476933 0.397351 0.113 Uiso 1 1 calc GR . . . .
C8 C 0.1921(4) 0.4011(4) 0.6851(3) 0.0864(12) Uani 1 1 d . . . . .
H8A H 0.127742 0.461920 0.706038 0.104 Uiso 1 1 calc R . . . .
H8B H 0.158616 0.376608 0.626930 0.104 Uiso 1 1 calc R . . . .
C9 C 0.8459(4) 0.5971(3) 0.5339(3) 0.0796(9) Uani 1 1 d . . . . .
H9A H 0.841519 0.664027 0.567965 0.119 Uiso 1 1 calc GR . . . .
H9B H 0.939105 0.597200 0.497994 0.119 Uiso 1 1 calc GR . . . .
H9C H 0.848240 0.534703 0.573209 0.119 Uiso 1 1 calc GR . . . .
C10 C 0.2104(7) 0.3106(6) 0.7501(4) 0.150(3) Uani 1 1 d . . . . .
H10A H 0.140960 0.317746 0.800736 0.181 Uiso 1 1 calc R . . . .
H10B H 0.200458 0.237750 0.723827 0.181 Uiso 1 1 calc R . . . .
C11A C 0.557(3) 0.1929(11) 0.5579(14) 0.048(3) Uani 0.5865 1 d D U P A 1
H11A H 0.473555 0.172590 0.521650 0.058 Uiso 0.5865 1 calc R . P A 1
C12 C 0.5913(3) 0.3129(2) 0.60943(16) 0.0513(6) Uani 1 1 d D U . . .
C13A C 0.6923(16) 0.1297(12) 0.5848(12) 0.071(4) Uani 0.5865 1 d D U P A 1
H13A H 0.705122 0.056026 0.568759 0.086 Uiso 0.5865 1 calc R . P A 1
C14A C 0.7972(14) 0.1826(9) 0.6338(9) 0.061(4) Uani 0.5865 1 d D U P A 1
H14A H 0.890160 0.149004 0.651979 0.074 Uiso 0.5865 1 calc R . P A 1
C11B C 0.763(2) 0.331(2) 0.6648(15) 0.045(4) Uani 0.4135 1 d D U P A 2
H11B H 0.803361 0.391457 0.694599 0.054 Uiso 0.4135 1 calc R . P A 2
C13B C 0.827(3) 0.2178(12) 0.6505(17) 0.052(3) Uani 0.4135 1 d D U P A 2
H13B H 0.923847 0.196657 0.673771 0.062 Uiso 0.4135 1 calc R . P A 2
C14B C 0.7390(18) 0.1476(14) 0.6022(13) 0.052(4) Uani 0.4135 1 d D U P A 2
H14B H 0.770735 0.075728 0.589598 0.062 Uiso 0.4135 1 calc R . P A 2


_geom_special_details            
;
 All esds (except the esd in the dihedral angle between two l.s. planes)
 are estimated using the full covariance matrix.  The cell esds are taken
 into account individually in the estimation of esds in distances, angles
 and torsion angles; correlations between esds in cell parameters are only
 used when they are defined by crystal symmetry.  An approximate (isotropic)
 treatment of cell esds is used for estimating esds involving l.s. planes.
;
loop_
_geom_bond_atom_site_label_1
_geom_bond_atom_site_label_2
_geom_bond_distance
_geom_bond_site_symmetry_2
_geom_bond_publ_flag
S1 O1 1.483(2) . ?
S1 N1 1.683(2) . ?
S1 C2 1.839(3) . ?
S2A C12 1.585(6) . ?
S2A C14A 1.701(11) . ?
S2B C12 1.525(8) . ?
S2B C14B 1.679(16) . ?
N1 C1 1.506(3) . ?
N1 C5 1.501(4) . ?
C1 C3 1.560(3) . ?
C1 C12 1.492(4) . ?
C2 C6 1.528(4) . ?
C2 C7 1.512(4) . ?
C2 C9 1.517(4) . ?
C3 C4 1.530(4) . ?
C3 C5 1.530(4) . ?
C3 C8 1.538(4) . ?
C4 C10 1.460(7) . ?
C8 C10 1.478(7) . ?
C11A C12 1.672(15) . ?
C11A C13A 1.44(2) . ?
C12 C11B 1.692(18) . ?
C13A C14A 1.324(11) . ?
C11B C13B 1.49(2) . ?
C13B C14B 1.346(13) . ?

loop_
_geom_angle_atom_site_label_1
_geom_angle_atom_site_label_2
_geom_angle_atom_site_label_3
_geom_angle
_geom_angle_site_symmetry_1
_geom_angle_site_symmetry_3
_geom_angle_publ_flag
O1 S1 N1 109.67(11) . . ?
O1 S1 C2 105.70(12) . . ?
N1 S1 C2 102.43(12) . . ?
C12 S2A C14A 93.0(6) . . ?
C12 S2B C14B 95.0(7) . . ?
C1 N1 S1 119.96(16) . . ?
C5 N1 S1 112.30(18) . . ?
C5 N1 C1 91.7(2) . . ?
N1 C1 C3 89.04(18) . . ?
C12 C1 N1 114.0(2) . . ?
C12 C1 C3 118.17(19) . . ?
C6 C2 S1 102.3(2) . . ?
C7 C2 S1 110.62(19) . . ?
C7 C2 C6 111.2(3) . . ?
C7 C2 C9 113.6(3) . . ?
C9 C2 S1 108.3(2) . . ?
C9 C2 C6 110.2(3) . . ?
C4 C3 C1 121.6(2) . . ?
C4 C3 C8 88.0(3) . . ?
C5 C3 C1 88.6(2) . . ?
C5 C3 C4 122.4(3) . . ?
C5 C3 C8 121.7(3) . . ?
C8 C3 C1 118.2(3) . . ?
C10 C4 C3 89.3(3) . . ?
N1 C5 C3 90.4(2) . . ?
C10 C8 C3 88.3(3) . . ?
C4 C10 C8 93.0(3) . . ?
C13A C11A C12 101.0(14) . . ?
S2A C12 C11A 113.4(8) . . ?
S2B C12 C11B 115.9(8) . . ?
C1 C12 S2A 125.0(3) . . ?
C1 C12 S2B 124.8(4) . . ?
C1 C12 C11A 121.5(8) . . ?
C1 C12 C11B 119.2(8) . . ?
C14A C13A C11A 116.0(15) . . ?
C13A C14A S2A 116.5(12) . . ?
C13B C11B C12 97.4(16) . . ?
C14B C13B C11B 117(2) . . ?
C13B C14B S2B 114.7(16) . . ?

_olex2_submission_special_instructions 'No special instructions were received'
